Reduced Compton Wavelength of Electron
Jump to navigation
Jump to search
Theorem
The Compton wavelength of the electron is:
\(\ds \lambdabar_\E\) | \(\approx\) | \(\ds 3 \cdotp 86159 \, 267 \times 10^{-13} \, \mathrm m\) | ||||||||||||
\(\ds \) | \(\approx\) | \(\ds 3 \cdotp 86159 \, 267 \times 10^{-11} \, \mathrm {cm}\) |
Symbol
- $\lambdabar_\E$
The symbol for the reduced Compton wavelength of the electron is $\lambdabar_\E$.
The $\LaTeX$ code for \(\lambdabar_\E\) is \lambdabar_\E
.
Proof
By definition, the reduced Compton wavelength $\lambdabar_\E$ of an electron is given as:
- $\lambdabar_\E = \dfrac {\lambda_\E} {2 \pi}$
where $\lambda_\E$ denotes the Compton wavelength of the electron.
Then we have:
\(\ds \lambda_\E\) | \(\approx\) | \(\ds 2 \cdotp 42631 \, 02386 \, 7(73) \times 10^{-12} \, \mathrm m\) | Compton Wavelength of Electron | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \lambdabar_\E\) | \(\approx\) | \(\ds \dfrac {2 \cdotp 42631 \, 02386 \, 7(73) \times 10^{-12} } {2 \pi} \, \mathrm m\) | |||||||||||
\(\ds \) | \(\approx\) | \(\ds 3 \cdotp 86159 \, 267 \times 10^{-13} \, \mathrm m\) | by calculation | |||||||||||
\(\ds \) | \(\approx\) | \(\ds 3 \cdotp 86159 \, 267 \times 10^{-11} \, \mathrm {cm}\) | by calculation |
$\blacksquare$
Sources
- 1964: Milton Abramowitz and Irene A. Stegun: Handbook of Mathematical Functions ... (previous) ... (next): $2$. Physical Constants and Conversion Factors: Table $2.3$ Adjusted Values of Constants
- which gives the mantissa as $3 \cdotp 861 \, 692$ with an uncertainty of $\pm 12$ corresponding to the $2$ least significant figures